Under certain circumstances, Voigt waves can propagate in a biaxial composite
medium even though the component material phases individually do not support
Voigt wave propagation. This phenomenon is considered within the context of the
strong--permittivity--fluctuation theory. A generalized implementation of the
theory is developed in order to explore the propagation of Voigt waves in any
direction. It is shown that the correlation length--a parameter characterizing
the distributional statistics of the component material phases--plays a crucial
role in facilitating the propagation of Voigt waves in the homogenized
composite medium